CAIE A-Level Further Math 3.3.4 Vertical circular motion
Practise vertical circular motion by combining energy with radial force equations to find speeds, tensions and contact reactions.
- Syllabus
- 2028–2030
- Course
- Further Mathematics 9231
- Level
- AS
Practise vertical circular motion by combining energy with radial force equations to find speeds, tensions and contact reactions.
A particle P of mass m is attached to one end of a light inextensible rod of length 3 a. An identical particle Q is attached to the other end of the rod. The rod is smoothly pivoted at a point O on the rod, where O Q=x. The system, of rod and particles, rotates about O in a vertical plane.
At an instant when the rod is vertical, with P above Q, the particle P is moving horizontally with speed u. When the rod has turned through an angle of 60∘ from the vertical, the speed of P is 2ag, and the tensions in the two parts of the rod, OP and OQ, have equal magnitudes.
Find x in terms of a.
For P:T+mgcos60∘=3a−xm×4ag
B1
For Q:T−mgcos60∘=xmvQ2
B1
Eliminate T:−mgcos60∘+3a−xm⋅4ag=mgcos60∘+xmvQ2
M1
3a−xm×4ag=1+(3a−x)2mx4ag4a(3a−x)=(3a−x)2+4ax,x2+2ax−3a2=0
M1
Solve to find x.
Obtain 3-term quadratic equation.
(x−a)(x+3a)=0,x=a
A1
5
Find u in terms of a and g.
Additional page
If you use the following page to complete the answer to any question, the question number must be clearly shown.
B1
KEs correct.
Energy changes from initial position:
Gain in KE of P:21m(4ag−u2)
Loss in KE of Q:21m((2u)2−vQ2)
Loss in GPE of P=mg(3a−x)(1−cos60∘)(=mga)
Gain in GPE of Q=mgx(1−cos60∘)(=21mga)
B1FT
GPEs correct.
21m(4ag−u2)−21m((2u)2−vQ2)=−mgx(1−cos60∘)+mg(3a−x)(1−cos60∘)
M1
Energy equation.
Simplify: 4ag−45u2+ag=agu2=516ag,u=545ag
A1
AEF
4